CMB, The Horizon Problem and a comment on BH's

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Discussion Overview

The discussion revolves around the Cosmic Microwave Background (CMB), the Horizon Problem, and related concepts in cosmology. Participants explore the implications of the CMB's omnipresence, the conditions of the universe during last scattering, and the effects of cosmic expansion on particle horizons.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants question whether the curvature of the universe or the speed of expansion imposes constraints on receiving CMB photons from last scattering.
  • There is a proposal that a closed universe might allow CMB radiation to be received indefinitely, akin to a toroidal model.
  • Others suggest that the CMB is everywhere due to its creation throughout the universe, with photons from different regions now reaching us as space expands.
  • Concerns are raised about the Horizon Problem, specifically whether regions of the universe have always receded from each other faster than the speed of light, preventing them from being in each other's particle horizon.
  • Some participants argue that after inflation, the universe became transparent, leading to regions being too far apart to ever be in contact again due to accelerating expansion.
  • There is a discussion about whether the CMB implies a finite universe and positive curvature, with differing opinions on the implications of the CMB's omnipresence.
  • Participants express uncertainty about the role of inflation in solving the Horizon Problem, with some viewing it as a necessary explanation while others remain skeptical.
  • Several participants emphasize that the CMB represents radiation from the early universe when it became transparent, and they discuss the implications of this for understanding thermal equilibrium.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the implications of the CMB's omnipresence, the nature of the Horizon Problem, or the role of inflation. Multiple competing views remain, particularly regarding the conditions of the universe during last scattering and the effects of cosmic expansion.

Contextual Notes

Participants express varying assumptions about the universe's finiteness, the nature of cosmic expansion, and the conditions during the early universe, which may affect their interpretations of the CMB and the Horizon Problem.

  • #31
Just to keep everything on track, my question is:

Given that the universe initially had "a small initial radius." were particles that now casually disconnected regions of the CMB within each others particle horizon? And if not, is it because they were separating at a speed close to, or greater than, c? (separating by expansion)
 
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  • #32
superg33k said:
How do you conclude this from the first statement?
Nice catch. I forgot the important assumption: in a spacetime in which physical length scales, l_{\rm phys} \propto a(t) (where a(t) is the scale factor) expand (monotonically) at a slower rate than the Hubble radius, d_{H} \propto H^{-1}, i.e.
\frac{d}{dt}\left(\frac{d_{H}}{l_{\rm phys}}\right) > 0
and if the physical separation between two points a and b at a time t* satisfies
l_{\rm phys}(t^*) > d_H(t^*)
then l_{\rm phys}(t) > d_H(t) for all t < t^*. From
\frac{d}{dt}\left(\frac{d_{H}}{l_{\rm phys}}\right) = \frac{d}{dt} \left(\frac{1}{aH}\right) = -\frac{\ddot{a}}{\dot{a}^2} > 0
we see that our assumption holds in all spacetimes for which \ddot{a}<0 -- non-inflationary spacetimes.
 
  • #33
Ok, the texts I have read didn't go into the horizon problem that mathsy but I think I got it. From what I gather you are saying that all points that are outside each others Hubble radius now have always been outside each others Hubble radius.

To apply this to the CMB I am going to assume that the 2 separate parts are outside each others Hubble radius which is why they are in casually disconnected regions of space. Thus they have always been outside each others Hubble radius. So they have been separating faster than c since the big bang?
 
  • #34
superg33k said:
Ok, the texts I have read didn't go into the horizon problem that mathsy but I think I got it. From what I gather you are saying that all points that are outside each others Hubble radius now have always been outside each others Hubble radius.
Yes, for non-inflationary spacetimes, this is correct.
To apply this to the CMB I am going to assume that the 2 separate parts are outside each others Hubble radius which is why they are in casually disconnected regions of space. Thus they have always been outside each others Hubble radius. So they have been separating faster than c since the big bang?
Yes.
 
  • #35
Excellent. Thanks for going through this all with me. I'm happy to say the horizon problem makes sense. Additionally I never realized that non-infamitory models required a constant rate of expansion of the scale factor, which makes sense also.
 
  • #36
superg33k said:
Excellent. Thanks for going through this all with me. I'm happy to say the horizon problem makes sense.
Great! Happy to help.
Additionally I never realized that non-infamitory models required a constant rate of expansion of the scale factor, which makes sense also.
I hope I didn't say this! By definition, non-inflationary spacetimes need only satisfy \ddot{a}<0. The scale factor in non-inflationary models is not necessarily constant -- for example, in a radiation dominated universe a(t) \sim t^{1/2}, whereas in a matter dominated one a(t) \sim t^{2/3}.
 
  • #37
bapowell said:
I hope I didn't say this!

Yep, your right, you didn't. An inequality became an equality in my head.
 

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